NGZF: Difference between revisions

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{{TAGDEF|NGZF|[integer]|set in accordance with {{TAG|PREC}}, {{TAG|NGZ}}, {{TAG|ENCUT}} and {{TAG|ENAUG}}}}
{{TAGDEF|NGZF|[integer]|set in accordance with {{TAG|PREC}}, {{TAG|NGZ}}, {{TAG|ENCUT}} and {{TAG|ENAUG}}}}


Description: {{TAG|NGZF}} sets the number of grid points in the "fine" FFT-grid along the first lattice vector.
Description: {{TAG|NGZF}} sets the number of grid points in the "fine" FFT grid along the first lattice vector.
----
----
On this "fine" FFT mesh the localized augmentation charges are represented if ultrasoft pseudopotentials (USPPs) or the PAW method are used. In case USPPs are used, the local potentials (exchange-correlation, Hartree-potential and ionic potentials) are also calculated on this "fine" FFT-mesh.
On this "fine" FFT mesh the localized augmentation charges are represented if ultrasoft pseudopotentials (USPPs) or the PAW method are used. In case USPPs are used, the local potentials (exchange-correlation, Hartree-potential, and ionic potentials) are also calculated on this "fine" FFT-mesh.


By default {{TAG|NGZF}} is set in accordance with the requested "precision"-mode ({{TAG|PREC}}), {{TAG|NGZ}}, and the plane wave kinetic energy cutoffs {{TAG|ENCUT}} and {{TAG|ENAUG}}:
By default {{TAG|NGZF}} is set in accordance with the requested "precision" mode {{TAG|PREC}}, {{TAG|NGZ}}, and the plane wave kinetic energy cutoffs {{TAG|ENCUT}} and {{TAG|ENAUG}}:


::{| cellpadding="5" cellspacing="0" border="1"
::{| cellpadding="5" cellspacing="0" border="1"
|{{TAG|PREC}} || {{TAG|NGZ}} || {{TAG|NGZF}}
|{{TAG|PREC}} ||align="center"| {{TAG|NGZ}} ||align="center"| {{TAG|NGZF}}
|-
|-
| Normal || 3/2&times;G<sub>cut</sub> || 2&times;{{TAG|NGZ}}
| Normal ||align="center"| 3/2&times;<math>G_{\rm cut}</math> ||align="center"| 2&times;{{TAG|NGZ}}
|-
|-
| Single || 3/2&times;G<sub>cut</sub> || {{TAG|NGZ}}
| Single (VASP.5) ||align="center"| 3/2&times;<math>G_{\rm cut}</math> ||align="center"| {{TAG|NGZ}}
|-
|-
| Accurate || 2&times;G<sub>cut</sub> || 2&times;{{TAG|NGZ}}
| Single (VASP.6) ||align="center"| 2&times;<math>G_{\rm cut}</math> ||align="center"| {{TAG|NGZ}}
|-
|-
| Low || 3/2&times;G<sub>cut</sub> || 3&times;G<sub>aug</sub>
| SingleN (VASP.6) ||align="center"| 3/2&times;<math>G_{\rm cut}</math> ||align="center"| {{TAG|NGZ}}
|-
|-
| Medium || 3/2&times;G<sub>cut</sub> || 4&times;G<sub>aug</sub>
| Accurate ||align="center"| 2&times;<math>G_{\rm cut}</math> ||align="center"| 2&times;{{TAG|NGZ}}
|-
|-
| High || 2&times;G<sub>cut</sub> || 16/3&times;G<sub>aug</sub>
| Low ||align="center"| 3/2&times;<math>G_{\rm cut}</math> ||align="center"| 3&times;<math>G_{\rm aug}</math>
|-
| Medium ||align="center"| 3/2&times;<math>G_{\rm cut}</math> ||align="center"| 4&times;<math>G_{\rm aug}</math>
|-
| High ||align="center"| 2&times;<math>G_{\rm cut}</math> ||align="center"| 16/3&times;<math>G_{\rm aug}</math>
|}
|}
where
where
:<math>E_{\rm cut}=\frac{\hbar^2}{2m_e}G_{\rm cut}^2 \qquad E_{\rm aug}=\frac{\hbar^2}{2m_e}G_{\rm aug}^2</math>
:<math>E_{\rm cut}=\frac{\hbar^2}{2m_e}G_{\rm cut}^2 \qquad E_{\rm aug}=\frac{\hbar^2}{2m_e}G_{\rm aug}^2</math>
with E<sub>cut</sub>={{TAG|ENCUT}} and E<sub>aug</sub>={{TAG|ENAUG}}.
with <math>E_{\rm cut}</math>={{TAG|ENCUT}} and <math>E_{\rm aug}</math>={{TAG|ENAUG}}.


Alternatively {{TAG|NGZF}} may be set to a specific value in the {{FILE|INCAR}} file.  
Alternatively, {{TAG|NGZF}} can be set to a specific value in the {{FILE|INCAR}} file.


== Related Tags and Sections ==
== Related tags and articles ==
{{TAG|NGX}},
{{TAG|NGX}},
{{TAG|NGY}},
{{TAG|NGY}},
Line 36: Line 40:
{{TAG|PREC}},
{{TAG|PREC}},
{{TAG|ENCUT}},
{{TAG|ENCUT}},
{{TAG|ENAUG}},
{{TAG|ENAUG}}
{{TAG|ENMAX}}


{{sc|NGZF|Examples|Examples that use this tag}}
{{sc|NGZF|Examples|Examples that use this tag}}
----


[[Category:INCAR]][[Category:Electronic Minimization]][[Category:Electronic Minimization Methods]]
[[Category:INCAR tag]][[Category:Projector-augmented-wave method]]

Latest revision as of 11:57, 17 October 2024

NGZF = [integer]
Default: NGZF = set in accordance with PREC, NGZ, ENCUT and ENAUG 

Description: NGZF sets the number of grid points in the "fine" FFT grid along the first lattice vector.


On this "fine" FFT mesh the localized augmentation charges are represented if ultrasoft pseudopotentials (USPPs) or the PAW method are used. In case USPPs are used, the local potentials (exchange-correlation, Hartree-potential, and ionic potentials) are also calculated on this "fine" FFT-mesh.

By default NGZF is set in accordance with the requested "precision" mode PREC, NGZ, and the plane wave kinetic energy cutoffs ENCUT and ENAUG:

PREC NGZ NGZF
Normal 3/2× NGZ
Single (VASP.5) 3/2× NGZ
Single (VASP.6) NGZ
SingleN (VASP.6) 3/2× NGZ
Accurate NGZ
Low 3/2×
Medium 3/2×
High 16/3×

where

with =ENCUT and =ENAUG.

Alternatively, NGZF can be set to a specific value in the INCAR file.

Related tags and articles

NGX, NGY, NGZ, NGXF, NGYF, PREC, ENCUT, ENAUG

Examples that use this tag